Electronic tube oscillation system



Feb. 23, 1954 M. MORRISON ELECTRONIC TUBE OSCILLATION SYSTEM 2 Sheets-Sheet l Filed Jan. 10, 1948 Feb. 23, 1954 My MORRISON 2,670,437

ELECTRONIC TUBE OSCILLATION SYSTEM Filed Jan. 10, 1948 2 Sheets-Sheet 2 I 68/0 V0171? MfAJl/RIMIA Patented Feb. 23, 1954 UNITED STATES PATENT OFFICE ELE'G'I RQN'IC- TUBE OSCILLATIO'N SYSTEM Montf ord Morrison, Rochester, N. Y.

Application January 19, 1948, Serial N 0. 1,595 8 Claims. (01. 250-36) The present invention relates generally to electron discharge tube oscillators, in particu-' lar to such oscillators when frequency stabilized, and to electric motor devices embodying such said oscillators.

The present invention is in part a continuation of patent application Serial No. 599,891, filed June 16, 1945, which issuedas Patent No. 2,443,691, June 22, 1948, and which was a continuation in part of application Serial No. 496,389, filed July 28, 1943, which issued as Patent No. 2,415,022, January 28, 1 947.

When the invention is employed as an oscillator, among the objects thereof are: to provide a novel method of causing coupling feed-backto the oscillatory circuit in oscillators; to provide frequency stabilization with variation plate circuit characteristics in oscillators; and particularly to provide frequency stabilization with variation in oscillator loading. Further and other objects, when the invention isemployed as an oscillatonii'lill be indicated and obvious to those skilled the art, upon reading the speci' fication in connection with the drawings hereof.

When the invention is" emplbyed as" an electric motor device, amongv the objects thereof are: to provide an electric motor device having a predetermined speedwhich may be fixed witha very high degree of accuracy; to provide con stancy in said speed with variation in the applied motor voltage; and particularly to provide constancy in said speed with variation in mechani cal loading of the motor. Further and other objects, when the invention is employed as an elec= tric motor device, will be indicated and obvious to those skilled in the art.

The nature of the invention resides important ly in the employment of two different oscillatory system's combined in tandem producing a; single frequency or producinga single speed in a motor.

One of said oscillatory systems is set to oscil= late, as an uncombincd oscillator, at a; frequency lower than the resonant frequency of its parallel oscillatory system, and the other of saidoscillatory systems" is set to oscillate, an uncom= bined oscillator, at a-- frequency higher than the resonant frequency of its parallel oscillatory system, and the resultant combined operation being obviously at' afrequen at which memo oscillators operate in tandem: The resulting combined structure provides the objects set forth above.

and exact description of the invention, it'- will be necessary topro'vide'a fuiierzcieareramrmore 2 exact theory of oscillator operation, as applied to the present invention, than is known to the applicant in published texts. The applicant will provide herein such extra-conventional theory as is thought to be pertinent.

The invention will be more fully understood from the following description and extra-conventional theory, when read in connection with the accompanying drawings, of which:

Fig. 1' is a circuit diagram of one embodiment of the invention in a simple form for clearness in explaining the basic structural principles of the invention;

Fig. 2 is a side view illustrating some detail of the type of motor mechanism employed in the embodiment described herein, and shows an eddy current disk and its magnet both being added to the element illustrated in the elevation shown in Fig. 1;

Fig. 3 shows a particular oscillator operating under condensive loading and Figs. 4 and 5, are other oscillator circuits which are used in illustrating the extra-conventional theory given herein;

Figs. 6, 7 and 8 are graphs relating to the oscillators shown in Figs. 3, 4, and 5 and;

Fig. 9 is a diagram illustrating the methods of making tests which define certain terms used in the extra-conventional theory presented herein.

Referring to Fig. I, l is an alternating current motor which may be, in practice, any one of the many types which can be made to operate synchronously with an applied alternating voltage. The motor may be of the inductor type with salient poles, a direct current field type with a' wound rotor having no salient poles, it may be of the phonic wheel type, or any other suitable substitution.

In the embodiment shown in Fig. 1, there is employed an inductor type motor with perma-' nent magnetic fields and of a type commonly used as a synchronous motor and as an alternating: current generator.

The stator member 2, Figs. 1 and 2, is of alaminated structureand has a permanent mag-' net member 3, which provides aconstant magnetic field for the motor. The teeth of the stator are so spaced angularly with reference to theteeth of the rotor 6, that the main magnetic circuit provided by the magnet 3, is first through coil' 5 and then through coil 6, as the rotor 6 re-' volves, and thus an alternating current is produ'ced'be'twee'n terminals 1 and 8.

The operation as described above is really that 3 of a generator, but of course, when alternating current is fed through windings 4 and 5, under proper conditions, the device will act as a motor.

Referring to Fig. 2, 23 is an eddy current disk fixed to motor shaft 22, and 24 is a magnet for disk 23, constituting a loading device for motor I, in the form of the well known eddy current brake.

Fig. 2, 25 is a variable speed motor having a speed regulator 26 and being connectable through switch 21 to regulator 26 and therefore to line 28.

The simplified illustration shown in Fig. 2 forms a motor-generator set with mechanical loading and will be understood by those familiar with the art to which the present invention appertains.

In the prior art it has been common practice to supply motor I, with alternating current amplified up to motor requirements from an electrically driven tuning fork. Under these conditions a high constancy of speed control can be obtained but only at a very high apparatus cost and with an excessive amount of weight. Further, under such conditions of operation, the motor has, like all synchronous motors, a distinct tendency to hunt, and while the mean speed may have a high precision of constancy, the instantaneous speed may, and often does, vary badly, thus making such a device unsuitable for certain fields of precise work where a complete absence of hunting and/or low apparatus cost is essential.

In Patent No. 2,415,022, the applicant disclosed a motor device which has a low apparatus cost, is entirely free from hunting and which may be firmly synchronized with minute injections of alternating current at, or near, the operating frequency. However motor devices constructed on the teachings of the above patent, when unsynohronized with a stable source of alternating current, sometimes, require a constant loading to operate at the highest constancy of speed, that is, under certain conditions of loading, the motor speed may change as much as a few tenths of one percent.

In the present device when operating unsynchronized, the speed of the motor and hence the frequency of the oscillator is entirely independent of mechanical and electrical loading, within the limit of breakdown torque of the motor, and the frequency of the system is the same for the motor stalled as for the motor running.

Also with the motor stalled and the system operating purely as an oscillator, the frequency of the system is independent of any reasonable electrical loading, resistive, inductive or condensive.

Such a result in a direct current motor or in an electronic tube oscillatory system, has not been discovered by the applicant in the prior art and is therefore considered by him as broadly new.

Further in the present system, the minimum requirement of synchronizing energy for firmly locking in the motor with an outside source of energy, under the conditions of operation, are not certain. However indications are that in a two stage system, an injected energy of the order of one millionth of the energy in the motor coils is sufficient and probably more than is necessary for good synchronization. Obviously the motor coils become the oscillator output coils when the system is employed as an oscillator.

Such a ratio as one million to one has not been approached by any two stage amplification system found in the prior art by the applicant.

Referring back to Fig. 1, the winding of electric motor I, is connected push-pull to the output of twin triodes 9, provided with a source I9, of plate supply voltage. The grids of twin triodes 9 are connected across a capacitance-inductance parallel oscillatory system II, the center I2 of which is connected with the cathodes of twin triodes 9.

The oscillatory system H is connected through feed-back variable resistors I3 and I4 and through capacitors I5 and I9, when switches I1 and I8 are closed, to the plates of twin triodes 9, which are connected push-pull to the windings 4 and 5.

Coils 4 and 5 may be shunted by an electrical load I9, and may be further shunted by a variable capacitor 29, by closing switch 2i.

Switches 29 and 39 are provided to connect and to disconnect the grids of twin triodes 9 to and from the oscillatory system II and to and from feed-back through resistors I3 and 54.

The entire circuit enclosed within dotted area A, is essentially that shown in the above patent and may be referred to as a retarded-oscillator or simply as oscillator A.

Within thedotted area B is a second complete oscillator which may be referred to as an advanced-oscillator, or simply as oscillator B.

Oscillator B has two variable plate resistors I94 and I95 connected push-pull to the output of twin triodes I99, also provided with plate power supply from source I9. The grids of twin triodes I99, may be connected across parallel oscillatory system. III, by closing switches I29 and I39. The center II2 of oscillatory system III is connected with the cathodes of twin triodes I99. r

The oscillatory system III is connected through feed-back variable resistors H3 and H4 and through capacitors H5 and H9, when switches II! and IIS are closed, to the plates of twin triodes I99, which are connected pushpull to the plate resistors I94 and E95.

Plate resistors I94 and I95 may be fully or partially shunted by variable capacitor I3I.

The output of oscillator B is resistance coupled to the oscillatory system II, of oscillator B, through capacitors I32 and I33 and through resistors I34 and I35. 7

A center tapped external source of alternating current I36 is provided with current limiting variable resistors I31 and I33 and switches I39 and I49. The center of source I33 is connected by lead M! to both oscillators at their ground potential points.

Alternating current source I36 may be connected to the grids of twin triodes 9 through leads I42 and I43, by means of switches I39 and I49; said source may be connected to the grids of twin triodes I99 through leads I44 and I45, by means of switches I39 and I49; and said source may be connected to the oscillatory system III, through leads I46 and I4], by means of switches I39 and I49.

It is believed that before the description of the operation of the invention is entered into it will be necessary to define certain terms as used herein and present some extra-conventional oscillator theory essential to a full understanding of the invention.

The following definitions establish the meanings of certain terms as used-herein.

omens? To tune a circuit means to set the LC of a circuit such that the line voltage and line current are phase.

In resonance may mean in "phase or 180'" out of phase depending upon the circuit referred to.

To set an oscillatory circuit means to the LC of the circuit to give the desired result. "The set LC may correspond to a value above, at, or below, the resonance frequency of the circuit.

The natural period of the circuit often referred to as the proper period at which an oscillator should work, is the period of pure exoenergic operation of the circuit and has no direct bearing on the endoenergic operation thereof, as will be shown hereinafter.

Exoenergic is the applicant's short term for the expression, Under conditions in which stored energy in the circuit is being given up." The word obviously corresponds to exothermic as used in describing chemical reactions.

Endoenergic is the applicants "short term for the expression, Under conditions in which energy is being supplied to the circuit? The word obviously corresponds to endothermic as used in describing chemical reactions.

'Endoenergic operation of any oscillatory system is commonly referred to as operation under forced oscillation, when the energy supplied is o'fthe same periodic character as the oscillations forced.

However impulse driven oscillators are under endoenergic operation for the duration of the impulse and under exoenergic operation during the absence of the impulse.

Forced oscillators providing output energy are under both endoenergic and exoenergic operation.

Fig. 3 shows a push-pull oscillator .having a resistance stabilized feed-back; the plate circuit has a center tapped resistor 30!, one set of switches 302 and 3.03 for introducing parallel variable capacitors 304 and 305 across the ends of resistor 30I, and a second .setof. switches 306 and 301 for introducing parallel variable capacitor 308 across the central position of resistor 30L When switches 306 and 30] are open and switches 302 and 303 are closed the diagram will be referred to as circuit C. When switches .306 and 301 are closed and switches 302 and303 are open the diagram will be referred to ascircuit D.

Fig. 4 shows "a push-pull oscillator having .a resistance stabilized feed-back and pure resistive loading in the platexcircuits. The diagram of this figure will :be referred to as circuit Fig. 5 shows a push-pull oscillator having :a resistance stabilized feed-back; the plate circuit has a split inductor 50! with a center tapped resistor 5.02 inserted between :the splitcoils. This part of the diagram will .be referred to as circuit F. The figure also 'hasa set of switches 503 and 504 for introducing parallel variable capacitor 505 across said split inductor; with 'switches503 and 504 closed the figure will "bemeferredto as circuit G.

The details .of Figs, "6, r: and s will .be.discussed under the operation of Figs. 13,14 and 5, but before these operations are taken.up,'it:is necessary t establish and define certa n fact rs wh h nter into said operations,- and whichsare expl ined "in connection with Rig, 9.

In Fig. 19, the part 'of the :diagram which lies entirely within the dotted area 1 1, constitutes a circuit identical with and While other oilcircuit mmces for purpmes of ilhistrae tion. The circuit E1 of the figure is provided with a set of switches .004 and 902, which may be thrown to disconnect the grids of the triodes from-the oscillatory system and connect the grids to a variable frequency center tapped source of variable alternating current 903. "The figure shows and defines three methods of measurement which will be referred to hereinafter, namely;

Grid voltage measurement, which is employed to measure voltage values and phase positions, under conditions in which no line current and ;no appreciable line dc-setting is permissible. This method is also used for obtainmg the phase angle between thevoltage and the current-in a parallel oscillatory system, under similar conditions. The "device within'dotted area aspeciaLl Al amplifier which is constructed to have negligible phase difierence between the input andoutput voltages for the frequencies employed, but "without any -necessarily high amplification. Such an amplifier may be constructed like a resistance :coupled output design, but with the coupling capacitor having a relatively large capacity .and the output resistor having an ohmic value relatively very high to that of the plate resistor. Phase difference between the input and output can be tested by means of an electronic-switch and a cathode ray oscilloscope.

Plate current measurements (the alternating current component thereof) are made by what may be called a resistance drop method. Referring to Fig. 9, the center tapped resistor 904 is a highly accurate non-inductive resistor which is left permanently in the e'ircuit and has suflicient resistance to give a usable reading on highresistance voltmeter V. M. The voltmeter resistance should be of the order of 100 times that of the resistor. Any direct current present in the resistor is prevented from entering the plate current measurement circuit 'by capacitor 1905. "The value of the current in the resistor is obviously determined by the voltmeter. 'For taking oscillograms and phase angie measurements of the current in resistor 904, an extremely high-fidelity interstage transformer 906, is employed having an input impedance of the order of 100 times that of resistor 904. .This arrangement should be checked .for phase difference, because all transformers sold .as high-fidelity types may -not have a zero phase difference between the input and output for the frequency used.

.Tube voltage measurements (the alternating current component thereof) are .made by a resistance drop" method .but across .a small percentage of the total resistance used, and if the total resistance used effects the circuit constants, the shunt resistance is either left in the circuit or an equivalent resistance is substituted, so that the operation of .the circuit without the measuring device is the same as when itis in use. Re- 'ferring to the circuit within the dotted area vJ, the total resistance betweenpoints 901 and 908 may be of the order of 1,000,000 .ohms, the effective resistance across the input of transformer '909, maybe of the order of :l0;00.0. Transformer 909 .is preferably an extremely high-'iidelity extremely small type such as go by such trade names as ouncers, inchers and so forth, and

:should have an input impedance of the .order of 1,000,000 :ohms, These combinations should always be checked for phasediiference. With 100 ,plate A. C. volts :good oscillograph deflections hurts :may be substituted iniits place, the illusare obtained through :an electronic switch, with the values given. Withthe circuit as connected in Fig. 9, the measurements are those of the circuit as an oscillator. Withswitches Bill and 902 thrown to connect independent A. C. source 903, the measurements are made on an amplifier and obviously phase angle measurements can be made on various parts of the circuit at any desired frequency.

Certain experimental facts will be established on the operation of Figs. 3, 4 and 5, based upon measurements taken by the circuits explained in Fig. 9.

Referring to Fig. 4, if the voltage values and phase angle are takenv of the parallel oscillatory circuit alone of circuit E, as a function of the applied frequency at a constant effective current, there is obtained the familiar resonance,- voltage curve ml and its phase angle curve I02, with reference to said current. If said oscillatory circuit is tuned to resonance at say X cycles independently and then put into circuit E, and the feed-back resistor properly adjusted, circuit E can be made to oscillate at X cycles or the resonant frequency of said oscillatory circuit.

, However if the same oscillatory circuit with its X cycle resonant tuning and with the same adjustment of feed-back resistors, is substituted in circuit F and the proper measurements made, it will be found that circuit F does not oscillate at X cycles, but at some higher frequency 80!, Fig. 8, and with a lower output with the same plate impedance, because it will be found that the grid voltage is lower.

Then if switches 503 and 504 are closed with low capacity adjustment of capacitor 565, it will be found that by increasing said capacity the frequency and grid voltage can be brought to the values of circuit E. Further adjustments of said capacity will lower the grid voltage. I

Now if the same oscillatory circuit with its X cycle resonant tuning and with the same adjustment of feed-back resistors is substituted in either circuit C or D, say in circuit D, it will be found that circuit D does not oscillate at X cycles, but at some lower frequency 60I, Fig. 6, and with a lower output with the same plate impedance, because it will be found that the grid voltage is lower.

It will be found that other factors, like amount of feed-backresistance, Q of oscillatory circuit at the frequency and voltage employed, and other factors which are beyond the scope essential to this disclosure, effect the oscillator frequency. A fuller more comprehensive mathematical discussion is reserved for a still broader disclosure in a separate application.

From the above tests it is obvious that the circuits C, D, E, F and G, can be made to oscillate at the same frequency by employing different LC values in the parallel oscillatory circuits.

If the parallel oscillatory circuit of circuit F is set so that circuit F oscillates at say 600 cycles, it will be found that the oscillatory circuit voltage values and their phase relation to the tube voltage (oscillatory circuit current) as a function of the circuit frequency, is represented by Fig. 8, in which the frequency corresponding to the line BOI, represents 600 cycles. Assume the phase lead shown to be, say 60, which is a common value. This means that the grid voltage lags the tube voltage by 60 and that the oscillatory circuit is not operating at the resonant point, but in the steep region of the high-frequency side.

By increasing the inductance of coil 50I, that is'by increasingthe phase angle between the 8 A. C. tube current and the A. 0. tube voltage, the line I moves to the right and the operating frequency is increased, and by decreasing the inductance of coil EBI, the operating frequency is decreased.

If coils 50I represent the operating winding of a synchronous type alternating current motor, the motor speed changes with change in frequency. That is, if circuit F, just discussed, represents the circuit A, Fig. 1, we have the operation, just discussed, applied to motor, which to this point is the disclosure of the patent referred to above.

It is obvious from the above that this much of the motor disclosure is subject to speed variation with load, a characteristic of direct current motors. While in the motor just described the variation can be made small--a few tenths of one percentit is, nevertheless, present.

As it has been indicated, circuits C, D and G, can be adjusted so that the grid voltage leads A. C. tube voltage at the operating frequency and say this frequency is 600 cycles and is represented by the line E85, Fig. 6. Obviously increasing the shunt capacity of these circuits, decreases the frequency thereof and decreasing the capacity increases the frequency, within proper operating limits.

Directions can now be given for completing the detailed structure and operation of Fig. 1. As an oscillator, the circuit is to operate, for example, at a frequency of 600 cycles and as a motor device the motor is to operate at 1800 R. P. M. with the number of poles shown in the figure.

First, the circuit in dotted area A is set up as shown in the area, with switches I1, I3, 20 and 30 open, and with circuit B out of operation. Source [36 is set to a frequency of 600 cycles and to a voltage which, through resistors I31 and I38, when switches I30 and I40 are closed upon leads I42 and I63, will produce the normal oscillatoroperation grid-voltage at the grids of tube 9.

The motor I is brought up to above 1800 R. P. M. by closing switch 21 and adjusting regulator 26, Fig. 2. After well known circuit ad.- justments, then switch 2'! can be opened and motor I will continue to run and at 1800 R. P. M. The phase angle between the A. 0. motor current and the A. C. tube voltage is taken and recorded tobe say 60.

Switches I30 and I00 are opened and switches IT, IS, 29 and 30 are closed. Oscillatory circuit I I and feed-back resistors are set to stable oscillator operation at 600 cycles with the motor operating (at 1800 R. P. M.), with some loading by eddy current disk 23 under suitable adjustment of magnet 24, Fig. 2.

Now oscillatory circuit I I, is set to a final position where the oscillator frequency and therefore the motor speed operate at a few tenths of one percent slow, that is under 600 cycles and under 1800 R. P. M., the best value has to be found by trial after complete adjustment of the entire system. The system is now operating in accordance with the data shown in Fig. 8.

Second, the circuit in dotted area B is set up as shown in. the area with switches H1, H8, I29 and'l3t open. Switches I39 and I40 are closed upon leads MS and it? and with source 535 operating at 600 cycles and at a suitable voltage, oscillatory circuit III is set so that the voltage thereof leads the line current (which will be tube voltage in the oscillator) by something of the magnitude of 15 (in some cases considerably less' suffices). Switches I39 andl40 are then 9 open d-and switches Ill, 8.123 and 130 are th n losed with circuit A out of operat on.

Capacitor I3! is then adjusted so that circuit B s illates at a frequency a f w tenths of on one. percent, faster than 600 cycles.

Circuits A and B are th n put into simultaneous operation, and by final adjustment of feedback resistors H3 and H4, the combined frequency of the two sys ems can be brou ht to exaotly the desired frequen y, which in the exomic is 60 cycles and hence the moto to actly .18 0 R. P. M.

From. the d scussion of ci cuits D and I", it is obvious to those skilled in the art that these circuits and other circu ts in h c y of these. an. be subst t t d fo c r u t B of F 1.

and I hereby disclosed such substitutions to be within the scope of the invention.

Under proper construction, setting and adjustments of the combined A and B circuits, the following are some of the operating characteristics which will be found present.

The motor speed is entirely independent of motor loading within the limits of the breakdown torque of the motor shaft.

The oscillation frequency is entirely independent of the output circuit loading, resistive, inductive or, capacitive, with-in operating limits; and in view of which, the frequency is independent of whether the motoris running or not.

The system is extremely sensitive to voltages, at or near the operating frequency, when injected into oscillatory circuit Hi. With 3 volteam- Peres. in motor coils .4 and 5, 3 micro-volt-arm pores injected into oscillatory circuit II I is more than is required for locking the system into synchronism with source I36, by closing switches I39 and M0 up n l ads I4 and I41. a c se in actual practice with switches I39 and MB closed and s-microwolteampcres being injected into oscillatory circuit l I l, with the result of firm synchronization, one of said switches could be opened without destroying good synchronization, so that the lower limit is indicated as being below 3 rn icrc-volt-amperes, or in other words the ratio of injected energy to the operating is greater than one to one million.

While directions have been given herein to retard the independent frequency of circuit B, a few tenths of one percent below the desired final operating frequency of the system and to advance the independent frequency of circuit A, afew tenths of one percent above the desired final operating frequency of the system, these values are given only as a set of operating conditions for a. starting point of final adjustment. These as well as other important adjustments should be. varied to find the values which give the best results under the conditions of desired operation.

In. the above. discussion of the operation of the circuit of Fig. 1 and its equivalent circuits, dire ions ha e. been iven for the advanc d 5- cilleier to be se at. a frequ ncy above normal ope ating f ency for the independent; prelim na y r uency v lue. y P d n an arbitrary end n ve plate load and settin th scillatory system to cause the desired frequency. This procedure causes the oscillatory system to operate at, a frequency below the resonant froquencv h re f. as. illust a ed n Fi However the application has found that in practical oscilla ors. one may start y ett ng the 9. Z1 Such the h normalp 195 QF QWQQY 9! 9 @131 $3. 5 n is b lowhe resonant frequency (say a few percent) of the 10 oscillatory system, and then it will be found that by adjustment of the feed-back resistors, the desired normal frequency can be obtained with or without condensive plate loading I31.

A common structural characteristic of the two systems or methods is obviously that the advanced oscillator operates with the in tandem frequency below the resonant frequency of its oscillatory system, and the retarded oscillator" operates with the in tandem frequency above the resonant frequency of its oscillatory system.

A species of the invention embodying the last escribed structure, employing no condensive loading in the plate circuit, comprises circuit A with circuit E substituted for circuit B of Fig. 1, that is, tandem coupled circuits as shown in Fig. 1, with circuit A as an output circuit, but with circuit B eliminated and with circuit E in its place. This combination will be referred to as circuit A-E.

An experimental study of circuit AE suggests an entirely different explanation of the theory of operation of the generic structure of the invention, and it is believed that this different theory of operation can be understood most readily by starting with circuits A and B as shown in Fig. 1, having been set to operate at say 600 cycles with the motor running at 18.00 R. P. M., as directed in the first instance.

The feed-back circuit of circuit A is opened so that no feed-back current is supplied to the grid-circuit thereof. The plate circuit capacitance of circuit B is reduced to substantially zero, by which procedure circuit B becomes equivalent to circuit E, and will be referred to as circuit E. With these settings circuit E is an oscillator having its output "rresistance-capacitance coupled to the input of circuit A, which, under the conditions stated is operating as a special sort of an amplifier.

The oscillatory system of circuit E is set such that the voltage thereof leads the feed-back current by a few degrees, as a preliminary figure subject to optimum setting say to 15, and then the feed-back resistances of oscillator circuit E are set to values which cause circuit E to oscillate at say 600 cycles and therefore amplifier and motor circuit A to operate at 600 cycles. The motor will run at 1800 R. P. M., if sufiicient voltage is produced at its coil terminals. When the motor is running under these conditions it operates as a conventional synchronous motor and therefore has a decided tendency to hunt.

The feed-back circuit of circuit E is now opened so that no feed-back current is supplied to the grid-circuit thereof, by which procedure circuit .E is put out of operation, except for such couling effect as its inactive circuits may have upon circuit A.

The feed-back circuit of oscillator circuit A is then closed and the feed-back resistances thereof are set to values which cause circuit A to oscillate at 600 cycles and the motor to run 9.111800 R. P. M.

Circuit A now operates in accordance with the teaching of the above cited patent. The frequency of oscillation of circuit A and the speed of the motor thereof can be set to be substantially independent of normal line voltage varia tions, but the frequency of oscillation, and therefore the speed of the motor, are slightly subject o mo or l adin both p tive and, negative.

In order to mak it. .clear what is meant-by positi e, loading and. by negative loading, assume that the eddy current brake oi. Fig 2,. is. sumo hated and that the motor of circuit A is operating at normal speed. If the speed of variable speed motor of Fig. 2, is regulated to a speed below said normal speed, the motor of circuit A is partially driving the variable speed motor and may be said to be operating under positive loadingor under positive torque. If the speed of variable speed motor of Fig. 2, is regulated to a speed above said normal speed, the motor of circuit A is partially driven by variable speed motor and may be said to be operating under negative loading or under negative torque.-

Normally when circuit A is set to operate independently at normal speed under normal loading, the addition of positive torque causes it to run slightly slower, and the addition of negative torque causes it to run slightly faster. However adjustments can be made to obtain different effects than those described.

Now with circuit A set to operate at normal frequency and the motor thereof operating at normal speed, in accordance with direction given above and with circuit E coupled thereto and set to operate at normal frequency when its feedback circuit is closed, said feed-back circuit is then closed and the tandem circuit operates at normal frequency and the motor operates at normal speed, if the directions have been properly carried out.

However it will be found that the frequency of the tandem circuit, and the speed of the motor, are not subject to variation with the addition of positive torque or with the addition of negative torque, within the break-down torque of the motor, and further, under usual preliminary adjustments the frequency of the tandem circuit, and the speed of the motor, tend to decrease with increase of line voltage and to increase with decrease of line voltage, rather than to go up and down with line voltage as is an outstanding characteristic of prior art oscillators and such motor devices.

While the setting and adjustment of circuit A can be made by those skilled in the art of audi-ofrequency resistance stabilized oscillators, some extra-conventional theory will be helpful in setting and adjusting circuit E, when it is employed to regulate circuit A.

In actual oscillators of the type represented by circuit E, the generated frequency depends importantly upon three factors-setting of the grid oscillatory circuit, the amount of feed-back current and the plate voltage. With the grid oscillatory circuit set for resonance at or near the proper operating frequency of the oscillator, the generated frequency varies inversely with the amount of feed-back current and inversely with the plate voltage.

Of the various embodiments of the invention so far constructed, best results have been obtained with the oscillation in the B circuit position, having its oscillatory element set for resonance at a frequency which will cause the grid voltage to lead the tube voltage by an angle of the order of about 15. Different values may be more satisfactory for different embodiments.

It will now be seen that the frequency of oscillator of circuit A varies with the plate voltage, and that oscillator of circuit E (also of circuits C and D) varies inversely with the plate voltage, 50 that the variation of plate voltage (line voltage variation) in one oscillator offsets the variation in the other oscillator, which constitutes frequency stabilization against the line voltage variation.

Returning to Fig. 1 under the operating condition that the feed-back circuit of circuit A is open and the tandem circuits are operating as oscillator circuit E driving circuit A as an amplifier. If the phase positions of the tube voltage in-circuits E and A are taken, it will be found as to be expected that they are 180 apart. If, however, the feed-back circuit of circuit A is closed, it will be found that the phase position of the tube voltage of circuit A is pushed ahead by the output voltage of circuit E, and that proper operation of the. tandem circuit is present when the two tubes voltages are out of phase by an angle less than 180.

In view of the above discussion the operation of the tandem circuit is also explained by the vector combinations of the two circuits reacting one upon the other, instead of from the pushpull frequency standpoint. However, the two apparently different physical explanations can be shown to be mathematically equivalent.

It is believed that the directions given herein are in such clear and exact terms as will enable those skilled in the art to make and use devicesembodying the spirit of the invention, and that a much greater amount of detail would destroy the conciseness required by the Rules of Practice, however some detail will be pointed out.

The circuits A and B are connected in tandem with circuit A being set to push ahead, if and when circuit B tends to lag behind the predetermined frequency and speed, and circuit A tends to withdrawal its normal contribution of energy to circuit B, if and when circuit B tends to advance in frequency beyond the predetermined frequency and speed, which of course is in fact an effect of circuit A holding back circuit B from advancing in frequency. Other explana tions of the operation can be given but it is be lieved that this one suffices for patent specification purposes.

The stability of the system in the presence of varying load is importantly caused by the feedback current from circuit A entering into the oscillatory circuit H l of circuit B. Feed-back current is, what its name implies, opposite in phase to the forward current in the circuit. As

- shown in Figs. 6 and 8, the grid voltage of 0s cillatory circuit Ill leads the grid voltage of os cillatory circuit H, but not enough to have a reversed phase position, that is, they are mostly positive at the same time, but the feed-back voltage from circuit A, when it flows through oscillatory circuit l l I, is mostly negative when the feed-back voltage from circuit B is positive, so that the feed-back current from circuit A is substracted (vectorially) from the feedback current from circuit B, when both currents flow through oscillatory circuit I I I. This means that if the feed-back current, from circuit A in oscillatory circuit l l l weakens, the resultant current therein is strengthened and circuit B takes more control of the system with an increased forward coupled feed into circuit A. If circuit 3 tends to run at a lower frequency the phase difference in the feed-back current (vector difference) increases the forward coupling. current from circuit B into oscillatory circuit H, pulling it up to the set frequency.

The above constitutes specific embodiments of the invention and the broader scope of the invention is pointed out with more particularity in the claims hereunder.

I claim:

1. In an electrical oscillation system, a first grid controlled electron discharge tube oscillator having in the plate circuit thereof a load subject to variation, said oscillator having a given fundamental isolation-operation frequency subject to variation with variation in said load, a second grid controlled electron discharge tube oscillator coupled to said first oscillator, said second oscillator having an isolation-operation frequency differing from said fundamental frequency by an amount greater than zero and substantially. less than the difierence between said fundamental frequency and a second harmonic thereof, and second said oscillator having a frequency regulation characteristic set to compensate frequency variation in first said oscillator due to variation in said load.

2. In an electrical oscillation system set to operate at a normal frequency under changing load, a first grid controlled electron discharge tube oscillator having in the plate circuit thereof a load subject to change, said oscillator having a frequency subject to change with change in said load, a second grid controlled electron discharge tube oscillator set to operate when isolated at frequency substantially less than twice said normal frequency, said second oscillator coupled to first said oscillator and said second oscillator having a frequency-change characteristic opposing frequency-changes in first said oscillator.

3. In an electrical oscillation system operating at a normal frequency, two grid controlled electron discharge tube oscillators, one of said oscillators having an effectively inductive plate load, said one oscillator having an uncoupled frequency set below said normal frequency, the other of said oscillators having an effectively capacitive load, said other oscillator having an uncoupled frequency set above said normal frequency, the difference between said frequency settings being substantially less than the difference between either of said frequencies and a second harmonic thereof, and two said oscillators coupled in tandem operating at said normal frequency.

4. An electrical oscillation system comprising a load circuit having a frequency determined by the combined operation of two grid controlled electron discharge tube oscillators operating in tandem, each of said oscillators having an oscillatory element in the grid circuit thereof, each of said elements being tuned to a different isolation-operation frequency, one of said oscillators including said load circuit, said load circuit having a circuit supplying feed-back current to the other of said oscillators, the element of said other oscillator being set to reflect said feed-back current back to said one oscillator through its oscillatory element at a phase angle opposing frequency shift in said oscillator, and both said oscillators being set at isolation-operation frequencies having a difference greater than zero and substantially less than the difference between either frequency and a second harmonic thereof.

5. In an electrical oscillation system having a terminal output circuit, two grid controlled electron discharge tube oscillators connected in tandem, each of said oscillators having a plate output circuit and an oscillatory element in the grid circuits thereof, the oscillatory element of one of said oscillators being set to operate at a frequency lower than the resonant frequency of said element, the oscillatory element of the other of said oscillators being set to operate at a frequency higher than the resonant frequency of element, the plate-output circuit of said one oscillator constituting said terminal output circuit, and the oscillatory element of said one oscillator constituting the plate-output circuit of said other oscillator.

65. in an electrical oscillation system having a terminal load, a first grid controlled electron discharge tube oscillator the output load of which constitutes said terminal load and the grid circuit of which includes an oscillatory element, said oscillatory element being set to operate at a first frequency, a second grid controlled electron discharge tube oscillator the output load of which includes said oscillatory element and the grid circuit of which includes a second oscillatory element, said second oscillatory element being set at a second frequency different from said first frequency, said two frequencies having a difference less than the ratio of 1 to 2, and said oscillators operating in tandem electrically coupled relation.

7. In an electrical oscillation system, two grid controlled electron discharge tube oscillators coupled in tandem, one of said oscillators having an inductive plate load, the other of said oscillators having a capacitive plate load, each of said oscillators having an oscillatory element in the grid control circuit thereof, said elements having different resonance frequencies, said frequencies differing by an amount greater than zero and substantially less than the difference between either one of said frequencies and a second harmonic thereof, and said system set to operate at a single oscillation frequency.

8. In an electrical oscillation system, two grid controlled electron discharge tube oscillators coupled in tandem, one of said oscillators connected to supply output current for said system, the other of said oscillators connected to supply input current to first said oscillator, each of said oscillators having oscillatory elements in the grid circuits thereof, said one oscillator having an inductive plate load, said other oscillator having a. capacitive plate load, said oscillators being set when isolated to operate at different frequencies, said frequencies differing by an amount greater than zero and substantially less than the difference between either one of said frequencies and a second harmonic thereof, and said two oscillators having an electrical coupling causing system operation at a single frequency.

MONTFORD MORRISON.

References Cited in the file of this patent UNITED STATES PATENTS Number Name Date 1,580,536 Rosenbaum Apr. 13, 1926 1,925,520 Buschbeck Sept. 5, 1933 2,098,386 Hansell Nov. 9, 1937 2,149,756 Arenberg et al Apr. 7, 1939 2,228,323 Mortley Jan. 14, 1941 2,248,481 Schuttig July 8, 1941 2,284,372 Crosby May 26, 1942 2,305,262 Lange Dec. 15, 1942 2,344,813 Goldstine Mar. 21, 1944 2,407,213 Tunick Sept. 3, 1946 2,423,103 Koechlin July 1, 1947 2,438,382 Born Mar. 23, 1943 2,445,933 Beste July 27, 1948 FOREIGN PATENTS Number Country Date 460,693 Great Britain Feb. 2, 1937 

